Update content - 2026-10-14

content/inbook/steinbuch11_advan_motion_contr_desig.md

@@ -54,7 +54,7 @@ Here, we focus on the control of linear time invariant electromechanical motion
 The dynamics of such systems are often dominated by the mechanics, such that:
 
 \begin{equation}
-G\_p(s) = \sum\_{i=1}^{N\_{rb}} \frac{c\_i b\_i^T}{s^2} + \sum\_{i=N\_{rb} + 1}^{N} \frac{c\_ib\_i^T}{s^2 + 2 \xi\_i \omega\_i s + \omega\_i^2}
+G\_p(s) = \sum\_{i=1}^{N\_{rb}} \frac{c\_i b\_i^T}{s^2} + \sum\_{i=N\_{rb} + 1}^{N} \frac{c\_ib\_i^T}{s^2 + 2 \zeta\_i \omega\_i s + \omega\_i^2}
 \end{equation}
 
 with \\(N\_{rb}\\) is the number of rigid body modes.